Heterojunction bipolar transistor having a germanium raised extrinsic base

ABSTRACT

Disclosed is a heterojunction bipolar transistor (“HBT”) including an intrinsic base in a SiGe layer. The HBT has a raised germanium extrinsic base over the SiGe layer. A base contact is situated over and contacting the raised germanium extrinsic base. An emitter is situated over the intrinsic base, and a collector is situated under the intrinsic base. The raised germanium extrinsic base has a reduced parasitic base-collector capacitance. The raised germanium extrinsic base is situated between a first dielectric layer and a second dielectric layer. Spacers are situated adjacent the second dielectric layer. The first dielectric layer can be a nitride based dielectric, the second dielectric layer can be an oxide based dielectric, and the spacers can be a nitride based dielectric.

The present application claims the benefit of and priority to aprovisional patent application titled “Silicon Germanium BipolarTransistor Having a Germanium Raised Extrinsic Base”, Ser. No.61/777,934, filed on Mar. 12, 2013. The disclosure in this provisionalapplication is hereby incorporated fully by reference into the presentapplication.

BACKGROUND

As semiconductor devices continue to decrease in size, optimal deviceoperation becomes more difficult to achieve. For example, when scalingadvanced bipolar transistors two factors are of primary importance: (1)scaling the vertical emitter-base-collector dimension to improve cutofffrequency (F_(t)) and DC current gain (β), and (2) scaling the lateraldimension of the bipolar transistor to improve the maximum frequency ofunity power gain (F_(max)) and the RF noise figure (Nf_(min)). Inbipolar transistors, lateral scaling has typically focused on reducingthe parasitic extrinsic base resistance (R_(bx)) and extrinsicbase-collector capacitance (C_(BC)).

In order to reduce the extrinsic base-collector capacitance, “raisedbase” techniques have been used. Over the last decade, conventionalraised base techniques have utilized processes having a separatedeposition step for creating an epitaxially grown extrinsic base regionthat connects the single-crystal intrinsic base region to the basecontact. In a typical raised base scheme the raised extrinsic basematerial is silicon (Si), and preferably polysilicon. Consequently, thesize of conventionally formed bipolar transistors is limited by thephysical properties of the epitaxial silicon raised extrinsic base.Moreover, fabrication of a silicon raised base often significantlyincreases manufacturing costs, and requires high temperature processingand is accompanied by difficulty in etching and forming the siliconraised base due to low etchant selectivity during fabrication.

SUMMARY

The present disclosure is directed to a heterojunction bipolartransistor having a germanium raised extrinsic base, substantially asshown in and/or described in connection with at least one of thefigures, and as set forth more completely in the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A presents an exemplary diagram showing a cross section of aconventional heterojunction bipolar transistor (“HBT”).

FIG. 1B presents an exemplary diagram showing a magnified view of across section of an intrinsic base region shown in FIG. 1A.

FIG. 2 shows a flowchart of a method for fabricating an HBT having agermanium raised extrinsic base, in accordance with an implementation ofthe present application.

FIG. 3A shows an initial HBT structure during an initial stage offabrication of an HBT according to one implementation of the presentapplication.

FIG. 3B shows an intermediate HBT structure during an intermediate stageof fabrication of an HBT according to one implementation of the presentapplication.

FIG. 3C shows an intermediate HBT structure during an intermediate stageof fabrication of an HBT according to one implementation of the presentapplication.

FIG. 3D shows an intermediate HBT structure during an intermediate stageof fabrication of an HBT according to one implementation of the presentapplication.

FIG. 3E shows a final HBT structure after fabrication of an HBTaccording to one implementation of the present application.

DETAILED DESCRIPTION

The following description contains specific information pertaining toimplementations in the present disclosure. The drawings in the presentapplication and their accompanying detailed description are directed tomerely exemplary implementations. Unless noted otherwise, like orcorresponding elements among the figures may be indicated by like orcorresponding reference numerals. Moreover, the drawings andillustrations in the present application are generally not to scale, andare not intended to correspond to actual relative dimensions.

As stated above, as semiconductor devices continue to decrease in size,optimal device operation becomes more difficult to achieve. For example,when scaling advanced bipolar transistors two factors are of primaryimportance: (1) scaling the vertical emitter-base-collector dimension toimprove cutoff frequency (F_(t)) and DC current gain (β), and (2)scaling the lateral dimension of the bipolar transistor to improve themaximum frequency of unity power gain (F_(max)) and the RF noise figure(Nf_(min)). In raised base bipolar transistors, lateral scaling hastypically focused on reducing the parasitic extrinsic base resistance(R_(bx)) and extrinsic base-collector capacitance (C_(BC)).

Over the last decade, conventional “raised base” techniques haveutilized processes having a separate deposition step for creating anepitaxially grown extrinsic base region that connects the single-crystalintrinsic base region to the base contact. However, as the lateraldistance between the extrinsic base and intrinsic base decreases,extreme proximity of dopants within the extrinsic base to the intrinsicbase can undesirably influence the effective size, shape and performanceof the intrinsic base. In all such raised base schemes the raisedextrinsic base material is silicon (Si), and preferably polysilicon.Consequently, the size of conventionally formed bipolar transistors islimited by the physical properties of the epitaxial silicon raisedextrinsic base.

The present inventive concepts utilize a raised extrinsic base made ofsubstantially pure germanium (Ge) to achieve smaller heterojunctionbipolar transistors (HBTs) than are possible using conventionalfabrication methods and without adding any new tooling relative to thatalready present in standard very large scale integration (VLSI)fabrication processes. The advantages of the present inventive conceptsmay include a reduced cost of fabrication due to lower processtemperatures and the elimination of one or more process steps related toconventional epitaxial silicon raised extrinsic base fabrication, areduced extrinsic base resistance, and an increased etchant selectivityduring fabrication.

FIG. 1A presents an exemplary diagram showing a cross section of aconventional HBT. FIG. 1A shows conventional HBT 100, includingsemiconductor substrate 110, which may be silicon, for example. However,semiconductor substrate 110 is not limited to silicon and may be anyappropriate substrate material, such as silicon-germanium (SiGe).Semiconductor substrate 110 may include collector 116 disposed betweenshallow trench isolation (STI) region 112 and STI region 114. SiGe layer130 may be grown on semiconductor substrate 110 and typically has agermanium concentration of between 20% and 30%. Oxide post 142 and oxidepost 144 may be deposited over SiGe layer 130 and an emitter 150 may beformed between and over oxide posts 142 and 144. Emitter 150 may beformed of N type single-crystal silicon or polysilicon, for example.Intrinsic base 136, which in the present implementation is asingle-crystal SiGe, is formed within intrinsic base region 120, and isdiscussed in more detail below regarding FIG. 1B. Extrinsic base region132 may be formed adjacent to oxide post 142 either within SiGe layer130, or alternatively, in an epitaxially grown silicon layer formed onSiGe layer 130 (not shown). In either case, extrinsic base region 132may be doped with a P type dopant, such as boron. Link base region 134may also include P type dopants and may electrically connect extrinsicbase 132 with intrinsic base region 120. Intrinsic base region 120 istypically a single-crystal SiGe. Silicide layer 152 may be formed overtop surfaces of SiGe layer 130 and emitter 150 to provide very lowresistance contact points for extrinsic base 132 and base contact 160,as well as for emitter 150.

In order to increase device density, the vertical and lateral dimensionsof HBTs must be decreased. However, simply decreasing the vertical andlateral dimensions of HBT 100 may have several undesired effects. Forexample, as the vertical dimension of HBT 100 is decreased, theshortened distance between extrinsic base region 132 and collector 116causes an increase in parasitic base-collector capacitance C_(BC),effectively reducing the maximum frequency at which HBT 100 can properlyoperate. In addition, as the lateral dimension of HBT 100 is decreasedthe distance d₁ between extrinsic base 132 and intrinsic base 136 alsodecreases. The close proximity of extrinsic base 132 means thatout-diffusion of dopants from extrinsic base 132 materially affect thedoping profile of intrinsic base 136. Such doping profile effects areshown in more detail in FIG. 1B.

FIG. 1B presents an exemplary diagram showing a magnified view of across section of intrinsic base region 120 shown in FIG. 1A. Intrinsicbase region 120 includes P type intrinsic base 136 and also shows threealternative emitter diffusion profiles and three alternative collectordiffusion profiles that may be alternatively formed. Emitter diffusionregion 122 a may represent an ideal emitter diffusion profile, in whichdopants from N type emitter 150 may diffuse evenly down into SiGe layer130. Similarly, collector diffusion region 124 a may represent an idealcollector diffusion profile, in which dopants from N type collector 116may diffuse evenly up into SiGe layer 130. In this ideal case, theeffective width of intrinsic base 136 may be at a maximum possiblewidth.

Emitter diffusion region 122 b and collector diffusion region 124 b mayrepresent actual emitter and collector diffusion regions, respectively,where extrinsic base region 132 is not too close to intrinsic base 136.Due to a small diffusion effect from P++ type dopants in link baseregion 134 and extrinsic base region 132, N type dopants from emitter150 above and collector 116 below do not fully diffuse to contact theentire width of intrinsic base 136, very slightly decreasing theeffective width of intrinsic base 136 from the ideal width.

Emitter diffusion region 122 c and collector diffusion region 124 c mayrepresent actual emitter and collector diffusion regions, respectively,where extrinsic base region 132 is too close to intrinsic base 136. Dueto a substantial diffusion effect from P++ type dopants in link baseregion 134 and extrinsic base region 132, N type dopants from emitter150 above and collector 116 below diffuse to a point considerably shortof contacting the entire width of intrinsic base 136, substantiallydecreasing the effective width of intrinsic base 136 from that of theideal width.

In an effort to overcome the above-described effects, a raised extrinsicbase of epitaxial silicon is formed on SiGe layer 130. Raising theextrinsic base above the SiGe layer decreases the parasiticbase-collector capacitance C_(BC) by further physically separating theextrinsic base from the collector. This also improves lateral scaling byincreasing the 3-dimensional straight-line distance between theextrinsic base and the intrinsic base. However, the presently knownraised base fabrication schemes utilize silicon for the raised extrinsicbase, limiting performance of the HBT by the physical properties ofsilicon, as discussed below.

According to the present inventive concepts, a specialized raisedextrinsic base made from substantially pure germanium (also referred toas a “raised germanium extrinsic base” herein) is utilized to furtherimprove HBT performance. For example, it has been found that holes indoped single-crystal germanium are approximately four times moreconductive than silicon with comparable doping, yielding approximatelyfour times lower resistance for the same dimensioned raised extrinsicbase. Moreover, there is evidence that polycrystalline germanium can bemore conductive than polysilicon, the polycrystalline germanium havingalmost metal-like conductive qualities. In addition, germanium is etchedby different chemicals than silicon, which allows near perfectselectivity when etching one in the presence of the other. Also,germanium has a far lower melting point than silicon (938° C. forgermanium versus 1414° C. for silicon), allowing lower processtemperatures than those required by silicon or SiGe based processes.This is a considerable advantage because as dimensions continue todecrease, process temperatures will also necessarily fall.

A method for fabricating an HBT having a substantially pure germaniumextrinsic raised base, according to the present inventive concepts, willnow be discussed with reference to FIG. 2 and FIGS. 3A, 3B, 3C, 3D and3E. FIG. 2 shows a flowchart of a method for fabricating an HBT having agermanium raised extrinsic base, in accordance with an implementation ofthe present application. FIG. 2 shows flowchart 200 having actions 210,220, 230, 240, 250 and 260. Action 210 may include depositing agermanium layer on a SiGe layer, and a first dielectric layer includinga first dielectric material on the germanium layer. For example, FIG. 3Ashows semiconductor substrate 310 including STIs 312 and 314. SiGe layer330 may be disposed on a top surface of semiconductor substrate 310.SiGe layer 330 may be formed by flowing silicon and germanium into areaction chamber at an appropriate rate, pressure and temperature untila desired thickness d₂ is reached. SiGe layer 330 may also be in situdoped with a P type dopant, such as boron or any suitable P type dopant.Once the desired thickness has been reached, the flow of silicon may bediscontinued while the flow of germanium is continued until germaniumlayer 370 is formed to a desired thickness d₃. Forming germanium layer370 in this manner allows continuous formation of both SiGe layer 330and germanium layer 370 and provides the additional benefit of producinga very low imperfection density at the SiGe/germanium interface. For thepurposes of this application, substantially pure germanium may beunderstood to correspond to a germanium concentration of approximately90% or greater. Germanium layer 370 may also be in situ P++ doped with aP type dopant such as boron.

As can be seen by doping profile 335, P type dopants are not initiallyintroduced in situ so that a very thin bottom portion of SiGe layer 330remains undoped. Doping concentrations may be quickly increased to forma concentration spike of P type dopants near the center of SiGe layer330 and then brought to a substantially zero value at the interfacebetween SiGe layer 330 and germanium layer 370. Doping concentrationsmay again be increased quickly as germanium layer 370 is grown.Intrinsic base 336 may also be formed in SiGe layer 330 by P type dopingat the appropriate time by any conventional method known to those ofordinary skill in the art. Next, dielectric layer 380 may be depositedon germanium layer 370. Dielectric layer 380 may be a nitride baseddielectric material, such as silicon nitride or silicon oxynitride, forexample.

Continuing to action 220, action 220 of flowchart 200 may includeetching away one or more portions of the germanium layer and one or moreoverlying portions of the first dielectric layer utilizing an emitterwindow mask to form an extrinsic base region. FIG. 3A shows HBT 300 aduring application of action 220 and after application of action 210.For example, emitter window mask 390 may be a photo-resist mask and maybe formed on dielectric layer 380 such that germanium layer 370 andoverlying dielectric layer 380 will be removed from all areas notadjacent to where the emitter will be formed. This may be achieved byutilizing a first etch chemistry which is selective to dielectric layer380 and somewhat selective to germanium and then switching to a secondetch chemistry which is highly selective to germanium, etching germaniumat a rate of at least 20× that of silicon. This allows for removal ofselect portions of germanium layer 370 to form extrinsic base 374 (shownin FIG. 3B) and extrinsic base 376 (shown in FIG. 3B) without riskingetching intrinsic base 336 formed in a top surface of SiGe layer 330.Such etch actions are shown by etchant 392. The shape of the emitterwindow mask is critical in that it opens up not only the area that willeventually serve as the emitter window, but also all regions of thesemiconductor substrate external to the HBT. This will allow forcomplete encapsulation of extrinsic bases 374 and 376 by subsequentdielectric deposition.

Continuing to action 230, action 230 of flowchart 200 may includedepositing a second dielectric layer including a second dielectricmaterial over the extrinsic base and the SiGe layer. FIG. 3B shows HBT300 b corresponding to HBT 300 a of FIG. 3A after application of action230. For example, dielectric layer 382 may provide a conformaldielectric layer over dielectric layer 380, on the sidewalls of each ofextrinsic bases 374 and 376, and over the entire exposed surface of SiGelayer 330. Dielectric layer 382 may be a dielectric material differentfrom that used in dielectric layer 380 and may also be etched by an etchchemistry different from dielectric layer 380, for example, an oxidebased dielectric, such as silicon oxide.

Action 240 of flowchart 200 may include forming spacers including thefirst dielectric material immediately adjacent the second dielectriclayer on each side of the extrinsic base. FIG. 3C shows HBT 300 ccorresponding to HBT 300 b of FIG. 3B after application of action 240.For example, spacers 384 may be formed by depositing a nitride baseddielectric material, such as silicon nitride or silicon oxynitride forexample, followed by an etch removing the nitride based dielectricmaterial from the top surfaces of dielectric layer 382 until only thespacers remain. It is important to point out that dielectric layer 380and spacers 384 may be formed from the same dielectric material, suchthat subsequent etching of dielectric layer 382 does not expose anyportion of extrinsic base 374 and extrinsic base 376, both of which aremade of substantially pure germanium. This is important becausegermanium is attacked by typical photoresist removal wet chemistryincluding hydrogen peroxide (H₂O₂), and also because subsequent dopantactivation by annealing is likely to melt extrinsic base 374 andextrinsic base 376, both of which are made of substantially puregermanium, requiring their complete encapsulation.

Continuing with action 250, action 250 of flowchart 200 may includeremoving the second dielectric layer over a top surface of the extrinsicbase and over a top surface of the SiGe layer such that the extrinsicbase remains completely enclosed by the first and second dielectriclayers. FIG. 3D shows HBT 300 d corresponding to HBT 300 c of FIG. 3Cafter application of action 250. For example, dielectric layer 382 maybe completely removed wherever it was disposed directly on SiGe layer330 and wherever it was disposed directly on dielectric layer 380, i.e.,over a top surface of extrinsic bases 374 and 376. The etch may becarried out until dielectric layer 380 is exposed on the top surface ofextrinsic bases 374 and 376. As can be seen, because the thickness ofthe portions of dielectric layer 382 applied to the sidewalls ofgermanium layer 370 is much greater in the vertical direction, thoseportions will remain after removal of the rest of dielectric layer 382.Thus, dielectric layer 380 encapsulates the top of extrinsic bases 374and 376, and dielectric layer 382 encapsulates each side of extrinsicbases 374 and 376. This is made possible by the etching protectionprovided by spacers 384 to the remaining portions of dielectric layer382. Where dielectric layer 382 is SiO₂, a suitable etchant process is ahydrochloric acid bath.

Extrinsic bases 374 and 376 may now survive the high thermal cyclespresent in the rest of a standard HBT process flow. In fact, it isexpected that extrinsic bases 374 and 376 will melt and re-crystallizeseveral times during the remaining process flow. This is advantageousbecause underlying SiGe layer 330 will act as a seed crystal layercausing extrinsic bases 374 and 376 to re-crystallize in single-crystalform over areas where SiGe layer 330 has a single-crystal structure.This process will be described in more detail regarding FIG. 3E below.

Turning to action 260, action 260 of flowchart 200 may include formingan emitter adjacent to and over the extrinsic base and over theintrinsic base formed in the SiGe layer. FIG. 3E shows HBT 300 ecorresponding to HBT 300 d of FIG. 3D after application of action 260.For example, emitter 350 may comprise N type polysilicon, and may beformed in an emitter window between extrinsic bases 374 and 376. Thus,emitter 350 may be formed adjacent to and over extrinsic bases 374 and376 and on intrinsic base 336 formed in SiGe layer 330. As discussedabove, extrinsic bases 374 and 376 may cyclically liquefy andre-crystallize during this and subsequent processes. Extrinsic bases 374and 376 may re-crystallize into one of several crystal structures,depending largely on the crystal structure of SiGe layer 330 at eachportion under extrinsic bases 374 and 376. For example, thesubstantially flat portions of SiGe layer 330 shown in FIGS. 3A through3E may be single-crystal SiGe due to a seed crystal effect fromunderlying semiconductor substrate 310. However, the mounded portions ofSiGe layer 330 may correspond to a polycrystalline formation due to thefact that STIs 312 and 314 do not provide a seed crystal from which togrow uniformly. Thus, portion 372 of extrinsic base 374 disposed oversingle-crystal SiGe may be single-crystal germanium, while portion 373of extrinsic base 374 disposed over polycrystalline SiGe may bepolycrystalline germanium.

In addition, as shown in FIG. 3E, a portion of dielectric layer 380 mayneed to be removed in order to connect base contact 360 with extrinsicbase 374. Once this portion of dielectric layer 380 is removed asilicide layer (not shown) may be formed on the exposed portion ofextrinsic base 374 in order to provide a very low resistance contactsurface for base contact 360. For completeness, also shown in FIG. 3Eare collector 316 corresponding to collector 116 in FIG. 1A, link base334 corresponding to link base 134 in FIG. 1A, and extrinsic (orparasitic) base-collector capacitance (C_(BC)). Conventional HBT processflows may be followed from this point forward.

Thus, the present inventive concepts utilize a raised extrinsic basemade of substantially pure germanium to reduce extrinsic (or parasitic)base-collector capacitance (C_(BC)) and to achieve smaller HBTs than arepossible using conventional fabrication methods and without adding anynew tooling relative to that already present in standard VLSIfabrication processes. Some of the advantages of the present inventiveconcepts include a reduced cost of fabrication due to lower processtemperatures and the elimination of one or more process steps related toconventional epitaxial silicon raised extrinsic base fabrication, areduced extrinsic base resistance, and an increased etchant selectivityduring fabrication.

From the above description it is manifest that various techniques can beused for implementing the concepts described in the present applicationwithout departing from the scope of those concepts. Moreover, while theconcepts have been described with specific reference to certainimplementations, a person of ordinary skill in the art would recognizethat changes can be made in form and detail without departing from thescope of those concepts. As such, the described implementations are tobe considered in all respects as illustrative and not restrictive. Itshould also be understood that the present application is not limited tothe particular implementations described above, but many rearrangements,modifications, and substitutions are possible without departing from thescope of the present disclosure.

The invention claimed is:
 1. A heterojunction bipolar transistor (“HBT”)comprising: an intrinsic base in a SiGe layer; a raised germaniumextrinsic base over said SiGe layer, a portion of said raised germaniumextrinsic base being situated on a mounded portion of said SiGe layer; abase contact situated over and contacting said raised germaniumextrinsic base; an emitter situated over said intrinsic base; acollector situated under said intrinsic base; said raised germaniumextrinsic base having a reduced parasitic base-collector capacitance;wherein said mounded portion of said SiGe layer is laterally adjacent tosaid intrinsic base in said SiGe layer.
 2. The HBT of claim 1 furthercomprising a first dielectric layer situated over said raised germaniumextrinsic base and under a portion of said emitter.
 3. The HBT of claim1 wherein said raised germanium extrinsic base is situated between afirst dielectric layer and a second dielectric layer.
 4. The HBT ofclaim 1 wherein said raised germanium extrinsic base is encapsulated bya first dielectric layer and a second dielectric layer.
 5. The HBT ofclaim 1 wherein a link base provides electrical connection between saidintrinsic base and said raised germanium extrinsic base.
 6. The HBT ofclaim 3 wherein said first dielectric layer comprises a nitride baseddielectric.
 7. The HBT of claim 3 wherein said second dielectric layercomprises an oxide based dielectric.
 8. The HBT of claim 3 furthercomprising a spacer adjacent said second dielectric layer.
 9. The HBT ofclaim 8 wherein said second dielectric layer comprises an oxide baseddielectric, and said spacer comprises a nitride based dielectric. 10.The HBT of claim 8 wherein said first dielectric layer comprises anitride based dielectric, said second dielectric layer comprises anoxide based dielectric, and said spacer comprises a nitride baseddielectric.
 11. A method for fabricating a heterojunction bipolartransistor (“HBT”) comprising: forming a germanium layer over a SiGelayer, said SiGe layer including an intrinsic base; forming a firstdielectric layer over said SiGe layer; etching portions of saidgermanium layer and said first dielectric layer to form a raisedgermanium extrinsic base, a portion of said raised germanium extrinsicbase being situated on a mounded portion of said SiGe layer; forming asecond dielectric layer over said raised germanium extrinsic base:wherein said mounded portion of said SiGe layer is laterally adjacent tosaid intrinsic base in said SiGe layer.
 12. The method of claim 11further comprising forming spacers adjacent said second dielectriclayer.
 13. The method of claim
 11. wherein said raised germaniumextrinsic base is encapsulated by said first dielectric layer and saidsecond dielectric layer.
 14. The method of claim 11, further comprisingforming an emitter over said intrinsic base.
 15. The method of claim 11,wherein a link base provides electrical connection between saidintrinsic base and said raised germanium extrinsic base.
 16. The methodof claim 11 , wherein said first dielectric layer comprises a nitridebased dielectric.
 17. The method of claim 11, wherein said seconddielectric layer comprises an oxide based dielectric.
 18. The method ofclaim 12, wherein said second dielectric layer comprises an oxide baseddielectric, and said spacers comprise a nitride based dielectric. 19.The method of claim 12, wherein said first dielectric layer comprises anitride based dielectric, said second dielectric layer comprises anoxide based dielectric. and said spacer comprises a nitride baseddielectric.
 20. The method of claim 14, wherein said intrinsic basecomprises a single-crystal SiGe, and said emitter comprises N typepolysilicon.